Using ÷_elements for CSRCSBEN?
Posted: 14 Jan 2014, 14:39
by Zamank
Hi All,
I am having difficulty using the divide element command for dividing a BC dipole to study the optics and CSR within the bend. Reading through the Elegant user manual, it says this should be possible, but I'm not so sure where I am going wrong.
Here is the command I am using BEFORE "&run_setup":
"÷_elements
name = BX21
!type = CSRCSBEN,
!exclude = NULL,
divisions = 5,
!maximum_length = 0,
clear = 0,
&end"
This is the dipole I am wanting to divide:
BX21 : CSRCSBEN,L= 5.492670000E-01, &
ANGLE="-5.407138055E-02 0.995 *", &
EDGE1_EFFECTS=1,E1= 0.000000000E+00, &
EDGE2_EFFECTS=1,E2="-5.407138055E-02 0.995 *", &
HGAP= 1.667500000E-02,FINT= 6.330000000E-01, &
SG_HALFWIDTH=2,SG_ORDER=1,STEADY_STATE=0,BINS=200, &
N_KICKS=20,INTEGRATION_ORDER=4,ISR=1,CSR=1
Re: Using ÷_elements for CSRCSBEN?
Posted: 23 Jan 2014, 17:44
by Zamank
Decided towards manually breaking up the bend into two pieces. I am still still slight fluctuations in the dispersion through out the system when I look at "etax". Wondering where I am going wrong here (if at all)?
Dipoles Divided************************************************************************************************************************************************************************************************
BX21A : CSRCSBEN,L= 0.274634, &
ANGLE="-0.02689077695348494", &
EDGE1_EFFECTS=1,E1= 0.000000000E+00, &
EDGE2_EFFECTS=0,E2="0", &
HGAP= 1.667500000E-02,FINT= 6.330000000E-01, &
SG_HALFWIDTH=2,SG_ORDER=1,STEADY_STATE=0,BINS=200, &
N_KICKS=10,INTEGRATION_ORDER=4,ISR=1,CSR=1
BX21B : CSRCSBEN,L= 0.274634, &
ANGLE="-0.02689077695348494", &
EDGE1_EFFECTS=0,E1="0", &
EDGE2_EFFECTS=1,E2="-0.02689077695348494 2.0 *", &
HGAP= 1.667500000E-02,FINT= 6.330000000E-01, &
SG_HALFWIDTH=2,SG_ORDER=1,STEADY_STATE=1,BINS=200, &
N_KICKS=10,INTEGRATION_ORDER=4,ISR=1,CSR=1
BX22A : CSRCSBEN,L= 0.274634, &
ANGLE="0.02689077695348494", &
EDGE1_EFFECTS=1,E1= "0.02689077695348494 2.0 *", &
EDGE2_EFFECTS=0,E2= "0", &
HGAP= 1.667500000E-02,FINT= 6.330000000E-01, &
SG_HALFWIDTH=2,SG_ORDER=1,STEADY_STATE=0,BINS=200, &
N_KICKS=10,INTEGRATION_ORDER=4,ISR=1,CSR=1
BX22B : CSRCSBEN,L= 0.274634, &
ANGLE="0.02689077695348494", &
EDGE1_EFFECTS=0,E1= "0", &
EDGE2_EFFECTS=1,E2= 0.000000000E+00, &
HGAP= 1.667500000E-02,FINT= 6.330000000E-01, &
SG_HALFWIDTH=2,SG_ORDER=1,STEADY_STATE=1,BINS=200, &
N_KICKS=10,INTEGRATION_ORDER=4,ISR=1,CSR=1
BX23A : CSRCSBEN,L= 0.274634, &
ANGLE= "0.02689077695348494", &
EDGE1_EFFECTS=1,E1= 0.000000000E+00, &
EDGE2_EFFECTS=0,E2= "0", &
HGAP= 1.667500000E-02,FINT= 6.330000000E-01, &
SG_HALFWIDTH=2,SG_ORDER=1,STEADY_STATE=0,BINS=200, &
N_KICKS=10,INTEGRATION_ORDER=4,ISR=1,CSR=1
BX23B : CSRCSBEN,L= 0.274634, &
ANGLE= "0.02689077695348494", &
EDGE1_EFFECTS=0,E1= "0", &
EDGE2_EFFECTS=1,E2= "0.02689077695348494 2.0 *", &
HGAP= 1.667500000E-02,FINT= 6.330000000E-01, &
SG_HALFWIDTH=2,SG_ORDER=1,STEADY_STATE=1,BINS=200, &
N_KICKS=10,INTEGRATION_ORDER=4,ISR=1,CSR=1
BX24A : CSRCSBEN,L= 0.274634, &
ANGLE="-0.02689077695348494", &
EDGE1_EFFECTS=1,E1="-0.02689077695348494 2.0 *", &
EDGE2_EFFECTS=0,E2= "0", &
HGAP= 1.667500000E-02,FINT= 6.330000000E-01, &
SG_HALFWIDTH=2,SG_ORDER=1,STEADY_STATE=0,BINS=200, &
N_KICKS=10,INTEGRATION_ORDER=4,ISR=1,CSR=1
BX24B : CSRCSBEN,L= 0.274634, &
ANGLE="-0.02689077695348494", &
EDGE1_EFFECTS=0,E1="0", &
EDGE2_EFFECTS=1,E2= 0.000000000E+00, &
HGAP= 1.667500000E-02,FINT= 6.330000000E-01, &
SG_HALFWIDTH=2,SG_ORDER=1,STEADY_STATE=1,BINS=200, &
N_KICKS=10,INTEGRATION_ORDER=4,ISR=1,CSR=1
Nominal ***************************************************************************************************************************************************************************************************
BX21 : CSRCSBEN,L= 5.492670000E-01, &
ANGLE="-5.407138055E-02 0.995 *", &
EDGE1_EFFECTS=1,E1= 0.000000000E+00, &
EDGE2_EFFECTS=1,E2="-5.407138055E-02 0.995 *", &
HGAP= 1.667500000E-02,FINT= 6.330000000E-01, &
SG_HALFWIDTH=2,SG_ORDER=1,STEADY_STATE=0,BINS=200, &
N_KICKS=20,INTEGRATION_ORDER=4,ISR=1,CSR=1
BX22 : CSRCSBEN,L= 5.492670000E-01, &
ANGLE=" 5.407138055E-02 0.995 *", &
EDGE1_EFFECTS=1,E1= "5.407138055E-02 0.995 *", &
EDGE2_EFFECTS=1,E2= 0.000000000E+00, &
HGAP= 1.667500000E-02,FINT= 6.330000000E-01, &
SG_HALFWIDTH=2,SG_ORDER=1,STEADY_STATE=0,BINS=200, &
N_KICKS=20,INTEGRATION_ORDER=4,ISR=1,CSR=1
BX23 : CSRCSBEN,L= 5.492670000E-01, &
ANGLE= "5.407138055E-02 0.995 *", &
EDGE1_EFFECTS=1,E1= 0.000000000E+00, &
EDGE2_EFFECTS=1,E2= "5.407138055E-02 0.995 *", &
HGAP= 1.667500000E-02,FINT= 6.330000000E-01, &
SG_HALFWIDTH=2,SG_ORDER=1,STEADY_STATE=0,BINS=200, &
N_KICKS=20,INTEGRATION_ORDER=4,ISR=1,CSR=1
BX24 : CSRCSBEN,L= 5.492670000E-01, &
ANGLE="-5.407138055E-02 0.995 *", &
EDGE1_EFFECTS=1,E1="-5.407138055E-02 0.995 *", &
EDGE2_EFFECTS=1,E2= 0.000000000E+00, &
HGAP= 1.667500000E-02,FINT= 6.330000000E-01, &
SG_HALFWIDTH=2,SG_ORDER=1,STEADY_STATE=0,BINS=200, &
N_KICKS=20,INTEGRATION_ORDER=4,ISR=1,CSR=1